Multiplex pulse time modulation system



June 9, 1953 P. F. M. GLoEss x-:r AL 2,641,699

- MULTIPLEX PULSE UME MobuLATIoN SYSTEM June 9, 1953 P. F. M. GLoEss ET AL 2,641,699

MULTIPLEX PULSE TIME MODULATION SYSTEM Filed March 25, 1949 2 Sheets-Sheet 2.

Patented June 9, 1953 UNITED STATES OFFICE MULTIPLEX PULSE TIME MODULATION SYSTEM Paul Franois Marie Gloess and Louis Joseph Libois, Paris, France Application March 25, 1949, Serial No. 83,302 In France March 27, 1948 In most hitherto known multiplex communica.- `tron systems, each ycommunication channel is assigned, for a given pulse-train, a time period longer than or at least equal to the value of the maximum displacement that may be undergone by the modulated pulse transmitting the intelligence, this pulse occurring at about the middle of this time-period when modulation is zero. So, whatever may the amplitude of the modulation be in the different communication channels, the average time-interval between two pulses connected with consecutive channels 'is constant.

It is, however, well-known that if a determined number of telephonie channels in operation are grouped, and if the amplitude of all the signals is analyzed at any moment, it will be found on the average that the respective amplitudes of lat least half the number of channels are zero, and that only a few among the remaining ones have maximum amplitudes. The `consequence is that in most presently known systems of transmission l' by time-displacement of pulses, the time-interval allotted to the transmission of a pulse train is not fully taken advantage of and includes considerably more dead periods than useful ones.

The present invention relates to special electronic devices for multiplex electric pulse transmission systems wherein the previously mentioned disadvantages are eliminated by the use of that type of modulation wherein a pulse of a channel is modulated by time-displacement from a position depending on the instantaneous position of the pulse of the preceding channel.

According to a first feature of the invention, each pulse is modulated from a position presenting a constant time-difference with the instantaneous position of the pulse of the preceding channel. In other words, the position Iof each pulse in relation to a pilot pulse is determined by the sum of the modulations undergone by this pulse and by the preceding pulses in the considered train of pulses, a convenient staggering in time being further added in order tol take in account the possibility of a zero modulation of one of several pulses.

According to another feature of the invention, every pulse is no more modulated about an average position, but from a position presenting a very small time-difference with the inst-antaneous position of the pulse immediately preceding it on the preceding channel, after having previ- 4 Claims. (Cl. Z50-27) ously transformed the modulation signals into unipolar signals by adding to them a rectified direct-current component of amplitude substantially proportional to that of said modulation signals, according to, a technique related to that of the noiseless type of motion-picture sound recording or of the floating carrier radiotelephonie transmission. 'Ihis very small time difference can be obtained in several ways, one

way being that of adding to each transformed modulation signal a lsmall direct current component so that, in case of zero modulation in one channel, the corresponding transformed modulation signal never takes a zero value. This is ntended to avoid overlapping of successive pulses in the said case of zero modulation in one channel. However such a provision is not always necessary, as it will be hereinafter seen from the description of some electronic pulses producing devices which are embodiments of the invention, a natural time delay between successive pulses occurs from the principle of functioning of the said devices, thanks to the finite time interval necessary to an electron beam for going from one position in space to another. In the latter case, the existence of a minimum delay between two successive pulses is thus guaranteed by the construction of the electronic device itself which generates the said pulses.

Other objects, characteristics and advantages of the invention will appear from the description of a few particular cases of embodiment, given as examples, but not implying a limitation of its scope.

The description is referred to the annexed drawings wherein:

Figure 1 shows a diagrammatical example of a device embodying characteristics of the invention.

Figure 2 is a diagram in connection with the description of Figure 1.

Figure 3 `shows another example of a -device including characteristics of the invention.

Figure 4 is a .diagram showing the signal obtained from the device on Figure 3.

Figure l shows an example of embodiment of the invention, in which a cathode-ray tube 54 is used. It has been supposed there that four communication channels are to be simultaneously transmitted, but it must be well understood that this small number has only Vbeen chosen for simplification of the drawing, and that the shown embodiment is not in the least limited to this number of channels.

ment 51 is connected with one of the terminals.

of a condenser 59 whose other terminal is earthed.

This condenser is negatively charged by an electronic tube vlill such as `a pentode, and is periodically discharged by a tube l5l which `causes a quick fly-back of the beam. Of course, arrangements may -be taken to switch the beam off duringthe y-back. So :a generator of saw-tooth Waves such as those shown on diagram of Figure 2 is obtained.

In the course of every sweeping from down to up, the beam strikes a rake-shaped electrode formed of .the parts or arms 62, 53, 6E, t5, 66 joined by a connection 61 to a load-resistance 68. A series of iive pulses represented on diagram of Figure 2 is thus obtained.

, Besides, tube 54 includes a manifold system of transversal deiiection, made of a common earthed plate 10 and of four distinct plates 1l, 12, 13 and 14, the whole system being of course possibly set deflection.

Lastly a target is disposed at the end of the tube 5d. This target is connectedon one hand to the earth by a load resistance 16, on the other hand to the control electrode Sua, of tube 60. Moreover, an earthed counter-target 11, intended to stop the part of the beam which' does not strike the target 15, has been represented, but it is obvious that this counter-target might be eliminated Without modication of the character of the deflection.

Plates for horizontal deection 1I, 12, 13 and 14 are respectively connected to the communication circuits through matching transformers 18, 19, 8!) and 8l and their respective voltages correspond at any moment to these channel modulation amplitudes.

It may be assumed for instance that the beam has just struck the electrode arm 63. ItV then passes between the horizontal deflection plates 12 and 1&3. The voltage of plate 12 being a function of the present modulation of the second communication channel, the beam undergoes a horizontal deflection which is itself a function of this modulation. It then more or less completely strikes the electrode 15, and so supplies to `the terminals of resistance 18 a voltage which is also a function of the considered channel instantaneous modulation. This voltage is `applied 'to the control electrode of tube Bil `and so controls the output of this tube. It consequently determines. the charging speed of condenser 59, i. e. the time in which the cathode beam reaches electrode arm 64 after leaving electrode arm 63.

rIhe pulse 82 Figure 2, produced by lthe beam when it strikes the collecting electrode arm 6l'. corresponding to the second communication channel is thenV delayed relatively to the pulse 83 Figure 2 of the rst channel by`a quantity which is a function of the instantaneous modulation of the second channel. Same phenomena Vsuccessively takes vplace for all the communication channels, and a system is so established, in which every pulse of a train is delayed relatively vup in front of or beyond the system of vertical to the immediately preceding one by a timeinterval depending upon the magnitude of the modulation applied at this instant to the channel to which the considered pulse corresponds.

On Figure 1, there has been represented in series with the connection between the channel transformer 18 and. the deflecting plate 1l a peak-levelling circuit consisting of a rectier 22 and of a condenser 25 in parallel with a resistance 28.

The function of this circuit is to transform alternating-current modulation signals from transformer 18, into modied modulation signals by adding to them a direct-current component substantially equal to the instantaneous envelope amplitude of said alternating-current signals.

VThepolarity of rectier 22 is chosen so `as to cause the modulation applied to the input side of transformer 18 to shift the average voltage of plate 'H in the positive direction and subsequently to decrease the deflection speed of the cathode ray beam and to increase the interval between pulse 83 `and the immediately preceding pulse, said interval being adjusted to a minimum value for the condition of zero modulation.

It is obvious that corresponding peak-levelling circuits may advantageously be added in series with the secondary windings of transformers 18, 863 and 8l corresponding to the other channels. In order to simplify the drawing, these circuits have not been represented on Figure l.

On Figure 3, a variant of the device on Figure l2 has been represented. Elements of this variant identical to those on Figure 1 bear same references.

Tube 84 includes a vertical saw-tooth sweeping system similar to that of tube 54 on Figure l.

In course of the sweeping from up to down, the electronic beam successively strikes the targets S5, 86, 81, 88, 89 and 9G.

Targets 86 to 89 are respectively connected to the communication channel circuits and targets and SE! are earthed. Every time the beam strikes one of these targets y85 to 90, it causes a secondary electron emission, the intensity of which is a function of the voltage applied to the struck target. The secondary electrons are collected on a collector electrode 9| connected lon one hand to a terminal of the load resistance 16, and on the other hand to the control electrode 60a, of tube Si).

If, for instance, the voltage applied to target 8S is considered, at the instant when the cathode beam strikes it, this voltage is a function of the instantaneous amplitude, at this instant, of the signals from the rst communicationV channel. Electrons collected on electrode 9| supply the control electrode of tube 6B with a voltage which is a function of this amplitude, and consequently condenser 59 is charged with Ia speed determined by that amplitude. The result is that the beam sweeps the target 86 with a velocity proportional to the instantaneous modulation of the communication channel corresponding to that target.

In its displacement between each of electrodes 85 to 9i), the beam strikes a further target 92 connected to the load-resistance 68 at the terminals of which a pulse signal such as that on diagram of Figure 4 is received, every pulse being delayed relatively to the immediately preceding one by a quantity proportional to the modulation of the channel to which the considered pulse corresponds.

.It will be noted on Figure 4 that the modulated pulse widths are variable. In fact, in its path between the consecutive targets 85 and 90, the initial velocity of the beam is that applied to it iby the target it has just left. So, the `pulse Widths themselves are an indication of the modulation they respectively carry, and the pulses are modulated in a complex manner both in time and in duration.

Through target 85, the fore-edge of the pilot pulse may be defined, and target 9U causes the back edge of the last channel pulse to appear.

In the same manner as already done in the case of Figure l, a peak-leveling circuit has been represented, by way of example, in series with the secondary winding of transformer 18. This circuit consists of rectiiier 22, condenser 25 and resistance 28. It is obvious that similar circuits may advantageously be added in series with each of the secondary windings of the other transformers 19, 80 and 8|.

It is obvious that the examples described have been given merely as illustrations, and that many variants and modications in shape and str-ucture of the described devices may be imagined Without going beyond the scope of the invention.

For instance, when using a cathode-ray tube for a large number of communication channels, it may be profitable to replace the linear saw-tooth sweeping system by a circular one, the beam being radially deiiected in a single direction as a function or" the instantaneous modulations of the different channels. Many -devices for embodying such a sweep-ing system are known, and it must be `understood that their use does not go beyond the scope of the invention.

We claim:

l. In a multiplex time division pulse communication system using recurrent groups of pulses, each group comprising a number of pulses at least equal to that of the `communication channels plus one, and wherein the individual modulation signals of a number of communication channels are represented by the time intervals between two successive pulses in each group, transmitting apparatus comprising a cathoderay beam tube including electro-optical means for flattening its beam in a direction parallel to a given rst direction, a iirst deflecting device for periodically deflecting said beam in a second direction perpendicular to said rst direction and bringing it back rapidly to its initial positon, a second deflecting device comprising pairs of electrodes, in number equal to that of communication channels for deilecting said beam in said rst direction, each pair of electrodes being submitted to a unipolar voltage obtained by adding to the alternating modulation signal voltage of one corresponding communication channel a rectiied direct-current component substantially proportional to the amplitude of said signal voltage, a rake-shaped electrode connected to a point at a iixed potential through a first resistor and arranged so as to be swept by the beam during its movement parallel to said second direction, a target connected to a point at a xed potential through a second resistor and arranged so as to be struck by the beam after its having swept said rake-shaped electrode, means for impressing voltage received at the terminals of said second resistor so as to influence deflection speed of above said first delecting device, and means for impressing voltage received at the terminals of said rst resistor upon a communication circuit.

2. Apparatus as in claim l, wherein a countertarget at a fixed potential is arranged side-to-side with the target in order to stop the part of the beam which does not strike said target.

3. Apparatus according to claim 1, wherein the first deflecting device comprises a condenser whose armatures assume a variable voltage difference under the action of a control -device fed from the second resistor.

4. Apparatus according to claim 1, wherein one of the electrodes of each pair of electrodes in second deflecting device is connected to a point at a fixed potential.

PAUL FRANQOIS MARIE GLOESS. LOUIS JOSEPH LLBOIS.

References Cited in the file of this patent UNITED STATES PATENTS FOREIGN PATENTS Country Date Great Britain Oct. 20, 1948 Number Number 

